Editing Fundamental interaction (section)

== Interactions ==
=== Gravity ===
{{Main|Gravity}}
''Gravitation'' is the weakest of the four interactions at the atomic scale, where electromagnetic interactions dominate.

Gravitation is the most important of the four fundamental forces for astronomical objects over astronomical distances for two reasons. First, gravitation has an infinite effective range, like electromagnetism but unlike the strong and weak interactions. Second, gravity always attracts and never repels; in contrast, astronomical bodies tend toward a near-neutral net electric charge, such that the attraction to one type of charge and the repulsion from the opposite charge mostly cancel each other out.<ref>{{cite news |last1=Siegel |first1=Ethan |title=What Is The Strongest Force In The Universe? |url=https://www.forbes.com/sites/startswithabang/2016/04/26/what-is-the-strongest-force-in-the-universe/ |access-date=22 March 2021 |work=[[Starts With a Bang]] |date=2016 |language=en}}</ref>

Even though electromagnetism is far stronger than gravitation, electrostatic attraction is not relevant for large celestial bodies, such as planets, stars, and galaxies, simply because such bodies contain equal numbers of protons and electrons and so have a net electric charge of zero. Nothing "cancels" gravity, since it is only attractive, unlike electric forces which can be attractive or repulsive. On the other hand, all objects having mass are subject to the gravitational force, which only attracts. Therefore, only gravitation matters on the large-scale structure of the universe.

The long range of gravitation makes it responsible for such large-scale phenomena as the structure of galaxies and [[black hole]]s and, being only attractive, it slows down the [[expansion of the universe]]. Gravitation also explains astronomical phenomena on more modest scales, such as [[planet]]ary [[orbit]]s, as well as everyday experience: objects fall; heavy objects act as if they were glued to the ground, and animals can only jump so high.

Gravitation was the first interaction to be described mathematically. In ancient times, [[Aristotle]] hypothesized that objects of different masses fall at different rates. During the [[Scientific Revolution]], [[Galileo Galilei]] experimentally determined that this hypothesis was wrong under certain circumstances—neglecting the friction due to air resistance and buoyancy forces if an atmosphere is present (e.g. the case of a dropped air-filled balloon vs a water-filled balloon), all objects accelerate toward the Earth at the same rate. Isaac Newton's [[law of Universal Gravitation]] (1687) was a good approximation of the behaviour of gravitation. Present-day understanding of gravitation stems from Einstein's [[General Theory of Relativity]] of 1915, a more accurate (especially for [[cosmology|cosmological]] masses and distances) description of gravitation in terms of the [[geometry]] of [[spacetime]].

Merging general relativity and [[quantum mechanics]] (or [[quantum field theory]]) into a more general theory of [[quantum gravity]] is an area of active research. It is hypothesized that gravitation is mediated by a massless [[Spin (physics)#Fermions and bosons|spin-2 particle]] called the [[graviton]].

Although general relativity has been experimentally confirmed (at least for weak fields, i.e. not black holes) on all but the smallest scales, there are [[alternatives to general relativity]]. These theories must reduce to general relativity in some limit, and the focus of observational work is to establish limits on what deviations from general relativity are possible.

Proposed [[extra dimensions]] could explain why the gravity force is so weak.<ref>{{cite web|url=http://home.web.cern.ch/about/physics/extra-dimensions-gravitons-and-tiny-black-holes|title=Extra dimensions, gravitons, and tiny black holes|date=20 January 2012|author=CERN}}</ref>

=== Electroweak interaction ===
{{Main|Electroweak interaction}}
[[Electromagnetism]] and weak interaction appear to be very different at everyday low energies. They can be modeled using two different theories. However, above unification energy, on the order of 100 [[GeV]], they would merge into a single electroweak force.

The electroweak theory is very important for modern [[cosmology]], particularly on how the [[universe]] evolved. This is because shortly after the Big Bang, when the temperature was still above approximately 10<sup>15</sup>&nbsp;[[Kelvin|K]], the electromagnetic force and the weak force were still merged as a combined electroweak force.

For contributions to the unification of the weak and electromagnetic interaction between [[particle physics|elementary particles]], Abdus Salam, Sheldon Glashow and Steven Weinberg were awarded the [[Nobel Prize in Physics]] in 1979.<ref>{{Citation |first=Sander |last=Bais |year=2005 |title=The Equations. Icons of knowledge |isbn=978-0-674-01967-6 |url-access=registration |url=https://archive.org/details/veryspecialrelat0000bais }} p.84</ref><ref>{{cite web|url=http://nobelprize.org/nobel_prizes/physics/laureates/1979/|title=The Nobel Prize in Physics 1979|publisher=The Nobel Foundation|access-date=2008-12-16}}</ref>

==== Electromagnetism ====
{{Main|Electromagnetism}}
Electromagnetism is the force that acts between [[electric charge|electrically charged]] particles. This phenomenon includes the [[electrostatic force]] acting between charged particles at rest, and the combined effect of electric and [[Magnetism|magnetic]] forces acting between charged particles moving relative to each other.

Electromagnetism has an infinite range, as gravity does, but is vastly stronger. It is the force that binds electrons to atoms, and it [[chemical bond|holds molecules together]]. It is responsible for everyday phenomena like [[light]], [[magnet]]s, [[electricity]], and [[friction]]. Electromagnetism fundamentally determines all macroscopic, and many atomic-level, properties of the [[chemical element]]s.

In a four kilogram (~1 gallon) jug of water, there is
<div class="center"><math> 4000 \ \mbox{g}\,\rm{H}_2 \rm{O} \cdot \frac{1 \ \mbox{mol}\,\rm{H}_2 \rm{O}}{18 \ \mbox{g}\,H_2 O} \cdot \frac{10 \ \mbox{mol}\,e^{-}}{1 \ \mbox{mol}\,H_2 O} \cdot \frac{96,000 \ \mbox{C}\,}{1 \ \mbox{mol}\,e^{-}} = 2.1 \times 10^{8} C \ \, \ </math></div>
of total electron charge. Thus, if we place two such jugs a meter apart, the electrons in one of the jugs repel those in the other jug with a force of
<div class="center"><math> {1 \over 4\pi\varepsilon_0}\frac{(2.1 \times 10^{8} \mathrm{C})^2}{(1 m)^2} = 4.1 \times 10^{26} \mathrm{N}.</math></div>

This force is many times larger than the weight of the planet Earth. The [[atomic nucleus|atomic nuclei]] in one jug also repel those in the other with the same force. However, these repulsive forces are canceled by the attraction of the electrons in jug A with the nuclei in jug B and the attraction of the nuclei in jug A with the electrons in jug B, resulting in no net force. Electromagnetic forces are tremendously stronger than gravity, but tend to cancel out so that for astronomical-scale bodies, gravity dominates.

Electrical and magnetic phenomena have been observed since ancient times, but it was only in the 19th century [[James Clerk Maxwell]] discovered that electricity and magnetism are two aspects of the same fundamental interaction. By 1864, [[Maxwell's equations]] had rigorously quantified this unified interaction. Maxwell's theory, restated using [[vector calculus]], is the classical theory of electromagnetism, suitable for most technological purposes.

The constant [[speed of light]] in vacuum (customarily denoted with a lowercase letter ''{{mvar|c}}'') can be derived from Maxwell's equations, which are consistent with the theory of special relativity. [[Albert Einstein]]'s 1905 theory of [[special relativity]], however, which follows from the observation that the [[speed of light]] is constant no matter how fast the observer is moving, showed that the theoretical result implied by Maxwell's equations has profound implications far beyond electromagnetism on the very nature of time and space.

In another work that departed from classical electro-magnetism, Einstein also explained the [[photoelectric effect]] by utilizing Max Planck's discovery that light was transmitted in 'quanta' of specific energy content based on the frequency, which we now call [[photon]]s. Starting around 1927, [[Paul Dirac]] combined [[quantum mechanics]] with the relativistic theory of [[electromagnetism]]. Further work in the 1940s, by [[Richard Feynman]], [[Freeman Dyson]], [[Julian Schwinger]], and [[Sin-Itiro Tomonaga]], completed this theory, which is now called [[quantum electrodynamics]], the revised theory of electromagnetism. Quantum electrodynamics and quantum mechanics provide a theoretical basis for electromagnetic behavior such as [[quantum tunneling]], in which a certain percentage of electrically charged particles move in ways that would be impossible under the classical electromagnetic theory, that is necessary for everyday electronic devices such as [[transistors]] to function.

==== Weak interaction ====
{{Main|Weak interaction}}
The ''weak interaction'' or ''weak nuclear force'' is responsible for some nuclear phenomena such as [[beta decay]]. Electromagnetism and the weak force are now understood to be two aspects of a unified [[electroweak interaction]] — this discovery was the first step toward the unified theory known as the [[Standard Model]]. In the theory of the electroweak interaction, the carriers of the weak force are the massive [[gauge boson]]s called the [[W and Z bosons]]. The weak interaction is the only known interaction that does not conserve [[parity (physics)|parity]]; it is left–right asymmetric. The weak interaction even [[CP-violation|violates CP symmetry]] but does [[CPT symmetry|conserve CPT]].

=== Strong interaction ===
{{Main|Strong interaction}}
The ''strong interaction'', or ''strong nuclear force'', is the most complicated interaction, mainly because of the way it varies with distance. The nuclear force is powerfully attractive between nucleons at distances of about 1 femtometre (fm, or 10<sup>−15</sup> metres), but it rapidly decreases to insignificance at distances beyond about 2.5 fm. At distances less than 0.7 fm, the nuclear force becomes repulsive. This repulsive component is responsible for the physical size of nuclei, since the nucleons can come no closer than the force allows.

After the nucleus was discovered in 1908, it was clear that a new force, today known as the nuclear force, was needed to overcome the [[Electrostatics|electrostatic repulsion]], a manifestation of electromagnetism, of the positively charged protons. Otherwise, the nucleus could not exist. Moreover, the force had to be strong enough to squeeze the protons into a volume whose diameter is about 10<sup>−15</sup> [[metre|m]], much smaller than that of the entire atom. From the short range of this force, [[Hideki Yukawa]] predicted that it was associated with a massive force particle, whose mass is approximately 100 MeV.

The 1947 discovery of the [[pion]] ushered in the modern era of particle physics. Hundreds of hadrons were discovered from the 1940s to 1960s, and an [[Regge theory|extremely complicated theory]] of hadrons as strongly interacting particles was developed. Most notably:
* The pions were understood to be oscillations of [[Vacuum expectation value|vacuum condensates]];
* [[Jun John Sakurai]] proposed the rho and omega [[vector boson]]s to be [[Yang–Mills theory|force carrying particles]] for approximate symmetries of [[isospin]] and [[hypercharge]];
* [[Geoffrey Chew]], Edward K. Burdett and [[Steven Frautschi]] grouped the heavier hadrons into families that could be understood as vibrational and rotational excitations of [[string theory|strings]].

While each of these approaches offered insights, no approach led directly to a fundamental theory.

[[Murray Gell-Mann]] along with [[George Zweig]] first proposed fractionally charged quarks in 1961. Throughout the 1960s, different authors considered theories similar to the modern fundamental theory of [[quantum chromodynamics|quantum chromodynamics (QCD)]] as simple models for the interactions of quarks. The first to hypothesize the gluons of QCD were [[Moo-Young Han]] and [[Yoichiro Nambu]], who introduced the [[quark color]] charge. Han and Nambu hypothesized that it might be associated with a force-carrying field. At that time, however, it was difficult to see how such a model could permanently confine quarks. Han and Nambu also assigned each quark color an integer electrical charge, so that the quarks were fractionally charged only on average, and they did not expect the quarks in their model to be permanently confined.

In 1971, Murray Gell-Mann and [[Harald Fritzsch]] proposed that the Han/Nambu color gauge field was the correct theory of the short-distance interactions of fractionally charged quarks. A little later, [[David Gross]], [[Frank Wilczek]], and [[David Politzer]] discovered that this theory had the property of [[asymptotic freedom]], allowing them to make contact with [[deep inelastic scattering|experimental evidence]]. They concluded that QCD was the complete theory of the strong interactions, correct at all distance scales. The discovery of asymptotic freedom led most physicists to accept QCD since it became clear that even the long-distance properties of the strong interactions could be consistent with experiment if the quarks are permanently [[color confinement|confined]]: the strong force increases indefinitely with distance, trapping quarks inside the hadrons.

Assuming that quarks are confined, [[Mikhail Shifman]], [[Arkady Vainshtein]] and [[Valentine Zakharov]] were able to compute the properties of many low-lying hadrons directly from QCD, with only a few extra parameters to describe the vacuum. In 1980, [[Kenneth G. Wilson]] published computer calculations based on the first principles of QCD, establishing, to a level of confidence tantamount to certainty, that QCD will confine quarks. Since then, QCD has been the established theory of strong interactions.

QCD is a theory of fractionally charged quarks interacting by means of 8 bosonic particles called gluons. The gluons also interact with each other, not just with the quarks, and at long distances the lines of force collimate into strings, loosely modeled by a linear potential, a constant attractive force. In this way, the mathematical theory of QCD not only explains how quarks interact over short distances but also the string-like behavior, discovered by Chew and Frautschi, which they manifest over longer distances.

=== Higgs interaction ===
Conventionally, the Higgs interaction is not counted among the four fundamental forces.<ref>{{cite web |title=fundamental force {{!}} Definition, List, & Facts |url=https://www.britannica.com/science/fundamental-interaction |website=Encyclopedia Britannica |access-date=22 March 2021 |language=en}}</ref><ref>{{cite web |title=The Standard Model |url=https://home.cern/science/physics/standard-model |website=CERN |access-date=22 March 2021 |language=en}}</ref>

Nonetheless, although not a [[gauge theory|gauge]] interaction nor generated by any [[diffeomorphism]] symmetry, the [[Higgs field]]'s cubic [[Yukawa interaction|Yukawa coupling]] produces a weakly attractive fifth interaction.  After [[spontaneous symmetry breaking]] via the [[Higgs mechanism]], Yukawa terms remain of the form
: <math>\frac{\lambda_i}{\sqrt 2} \bar{\psi} \phi' \psi = \frac{m_i}{\nu} \bar{\psi} \phi' \psi</math>,
with Yukawa coupling <math>\lambda_i</math>, particle mass <math>m_i</math> (in [[Electronvolt|eV]]), and Higgs [[vacuum expectation value]] {{val|246.22|u=GeV}}.  Hence coupled particles can exchange a [[virtual particle|virtual]] Higgs boson, yielding [[Yukawa interaction#Classical potential|classical potentials]] of the form
: <math>V(r) = - \frac{m_i m_j}{m_{\rm H}^2} \frac{1}{4\pi r} e^{-m_{\rm H}\, c\, r/\hbar}</math>,
with Higgs mass {{val|125.18|u=GeV}}. Because the [[reduced Compton wavelength]] of the [[Higgs boson]] is so small ({{val|1.576e-18|u=m}}, comparable to the [[W and Z bosons]]), this potential has an effective range of a few [[attometer]]s.  Between two electrons, it begins roughly 10<sup>11</sup> times weaker than the [[weak interaction]], and grows exponentially weaker at non-zero distances.

=== Beyond the Standard Model ===
{{main|Physics beyond the Standard Model}}
{{See also|Elementary particle#Beyond the Standard Model}}

The fundamental forces may become unified into a single force at very high energies and on a minuscule scale, the [[Planck scale]].<ref>{{Cite news|url=http://www.symmetrymagazine.org/article/the-planck-scale|date=2016-05-16 |last= Shivni | first= Rashmi  | title=The Planck scale|work=symmetry magazine|publisher= Fermilab/SLAC |access-date=2018-10-30|language=en}}</ref> [[Particle accelerator]]s cannot produce the enormous energies required to experimentally probe this regime. The weak and electromagnetic forces have already been unified with the [[electroweak interaction|electroweak theory]] of [[Sheldon Glashow]], [[Abdus Salam]], and [[Steven Weinberg]], for which they received the 1979 Nobel Prize in physics.<ref>{{Cite web|url=https://www.nobelprize.org/prizes/physics/1979/glashow/auto-biography/|title=The Nobel Prize in Physics 1979|website=NobelPrize.org|language=en-US|access-date=2018-10-30}}</ref><ref>{{Cite web|url=https://www.nobelprize.org/prizes/physics/1979/salam/biographical/|title=The Nobel Prize in Physics 1979|website=NobelPrize.org|language=en-US|access-date=2018-10-30}}</ref><ref>{{Cite web|url=https://www.nobelprize.org/prizes/physics/1979/weinberg/auto-biography/|title=The Nobel Prize in Physics 1979|website=NobelPrize.org|language=en-US|access-date=2018-10-30}}</ref> 
Numerous theoretical efforts have been made to systematize the existing four fundamental interactions on the model of electroweak unification.

[[Grand Unified Theories]] (GUTs) are proposals to show that the three fundamental interactions described by the Standard Model are all different manifestations of a single interaction with [[symmetry (physics)|symmetries]] that break down and create separate interactions below some extremely high level of energy. GUTs are also expected to predict some of the relationships between constants of nature that the Standard Model treats as unrelated, as well as predicting [[gauge coupling unification]] for the relative strengths of the electromagnetic, weak, and strong forces.

A so-called [[theory of everything]], which would integrate GUTs with a quantum gravity theory face a greater barrier, because no quantum gravity theories, which include [[string theory]], [[loop quantum gravity]], and [[twistor theory]], have secured wide acceptance. Some theories look for a graviton to complete the Standard Model list of force-carrying particles, while others, like loop quantum gravity, emphasize the possibility that time-space itself may have a quantum aspect to it.

Some theories beyond the Standard Model include a hypothetical [[fifth force]], and the search for such a force is an ongoing line of experimental physics research. In [[supersymmetric]] theories, some particles acquire their masses only through supersymmetry breaking effects and these particles, known as [[Moduli (physics)|moduli]], can mediate new forces. Another reason to look for new forces is the discovery that the [[expansion of the universe]] is accelerating (also known as [[dark energy]]), giving rise to a need to explain a nonzero [[cosmological constant]], and possibly to other modifications of [[general relativity]]. Fifth forces have also been suggested to explain phenomena such as [[Charge parity|CP]] violations, [[dark matter]], and [[dark flow]].